Search results for "Nucleon"

showing 10 items of 1041 documents

QUASIPARTICLE CALCULATIONS FOR THE THREE-NUCLEON SYSTEM

1972

Publisher Summary This chapter discusses the quasiparticle calculations for the three-nucleon system. There are three methods for solving the integral equations for the three-body problem with local two-body potentials; one method consists of the direct solution of the Faddeev equations, and the other two methods make different use of the quasiparticle idea that is based on the splitting of the occurring two-body potentials into a sum of separable terms and a rest potential. The chapter describes the term “form factors” and “coupling strengths.” A similar splitting is obtained for the T-matrices Tγ. With its help, it is possible to transform the Faddeev-type equations for the three-body tra…

PhysicsMomentumFaddeev equationsClassical mechanicsSimultaneous equationsQuantum mechanicsQuasiparticleNucleonIntegral equationConnection (mathematics)Resolvent
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(γ,2N) reaction inC12

1995

The $^{12}$C(\ensuremath{\gamma},pn) and $^{12}$C(\ensuremath{\gamma},pp) reactions have been measured for photon energies between 80 and 157 MeV using a photon tagging spectrometer and plastic scintillator detectors. The overall energy resolution was \ensuremath{\sim}7 MeV, sufficient to determine the initial shells of the emitted nucleons. Corrections were made for solid angle and threshold effects by means of Monte Carlo simulations. For the (\ensuremath{\gamma},pn) reaction both the missing energy and recoil momentum distributions are largely consistent with a two-nucleon absorption process on p-shell an sp nucleon pairs. For the much smaller $^{12}$C(\ensuremath{\gamma},pp) cross secti…

PhysicsMomentumNuclear and High Energy PhysicsPhotonMissing energyRecoilNuclear TheoryAbsorption (logic)Atomic physicsScintillatorNuclear ExperimentNucleonEnergy (signal processing)Physical Review C
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Studies of pear-shaped nuclei using accelerated radioactive beams

2013

There is strong circumstantial evidence that certain heavy, unstable atomic nuclei are ‘octupole deformed’, that is, distorted into a pear shape. This contrasts with the more prevalent rugby-ball shape of nuclei with reflection-symmetric, quadrupole deformations. The elusive octupole deformed nuclei are of importance for nuclear structure theory, and also in searches for physics beyond the standard model; any measurable electric-dipole moment (a signature of the latter) is expected to be amplified in such nuclei. Here we determine electric octupole transition strengths (a direct measure of octupole correlations) for short-lived isotopes of radon and radium. Coulomb excitation experiments we…

PhysicsMultidisciplinaryIsotopeta114010308 nuclear & particles physicsNuclear TheoryNuclear structureCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physics0103 physical sciencesAtomic nucleusQuadrupolePhysics::Accelerator PhysicsNeutronNuclidePhysics::Atomic PhysicsAtomic physics010306 general physicsNucleonNuclear Experiment
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A triplet of differently shaped spin-zero states in the atomic nucleus 186Pb

2000

Understanding the fundamental excitations of many-fermion systems is of significant current interest. In atomic nuclei with even numbers of neutrons and protons, the low-lying excitation spectrum is generally formed by nucleon pair breaking and nuclear vibrations or rotations. However, for certain numbers of protons and neutrons, a subtle rearrangement of only a few nucleons among the orbitals at the Fermi surface can result in a different elementary mode: a macroscopic shape change. The first experimental evidence for this phenomenon came from the observation of shape coexistence in 16O (ref. 4). Other unexpected examples came with the discovery of fission isomers and super-deformed nuclei…

PhysicsMultidisciplinaryNuclear TheoryNuclear structuremedicine.anatomical_structureAtomic orbitalAtomic nucleusmedicineNeutronAlpha decayAtomic physicsNuclear ExperimentSpin (physics)NucleonNucleusNature
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Superallowed Gamow-Teller decay of the doubly magic nucleus $^{100}$Sn

2012

Expérience au GSI; The shell structure of atomic nuclei is associated with 'magic numbers' and originates in the nearly independent motion of neutrons and protons in a mean potential generated by all nucleons. During b1-decay, a proton transforms into a neutron in a previously not fully occupied orbital, emitting a positron-neutrino pair with either parallel or antiparallel spins, in a Gamow-Teller or Fermi transition, respectively. The transition probability, or strength, of a Gamow-Teller transition depends sensitively on the underlying shell structure and is usually distributed among many states in the neighbouring nucleus. Here we report measurements of the half-life and decay energy fo…

PhysicsMultidisciplinaryProton010308 nuclear & particles physicsProton decayNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta decayNuclear physicsDecay energy0103 physical sciencesAtomic nucleusPhysical SciencesFysikNeutronAtomic physics010306 general physicsNucleonNuclear ExperimentRadioactive decay
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Gamma/neutron competition above the neutron separation energy in delayed neutron emitters

2014

To study the β-decay properties of some well known delayed neutron emitters an experiment was performed in 2009 at the IGISOL facility (University of Jyvaskyla in Finland) using Total Absorption -ray Spectroscopy (TAGS) technique. The aim of these measurements is to obtain the full β-strength distribution below the neutron separation energy (Sn) and the γ/neutron competition above. This information is a key parameter in nuclear technology applications as well as in nuclear astrophysics and nuclear structure. Preliminary results of the analysis show a significant γ-branching ratio above Sn. © Owned by the authors, published by EDP Sciences, 2014.

PhysicsNeutron emissionPhysicsQC1-999Binding energyNuclear TheoryNuclear physicsNuclear astrophysicsGamma spectroscopyNeutronNucleonNuclear ExperimentDelayed neutronRadioactive decayEPJ Web of Conferences
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Shadowing in Inelastic Nucleon-Nucleon Cross Section?

2020

Experimental results of inclusive hard-process cross sections in heavy-ion collisions conventionally lean on a normalization computed from Glauber models where the inelastic nucleon-nucleon cross section $\sigma_{\rm nn}^{\rm inel}$ -- a crucial input parameter -- is simply taken from proton-proton measurements. In this letter, using the computed electro-weak boson production cross sections in lead-lead collisions as a benchmark, we determine $\sigma_{\rm nn}^{\rm inel}$ from the recent ATLAS data. We find a significantly suppressed $\sigma_{\rm nn}^{\rm inel}$ relative to what is usually assumed, show the consequences for the centrality dependence of the cross sections, and address the phe…

PhysicsNormalization (statistics)Nuclear TheoryEikonal equationElectroweak interactionHigh Energy Physics::PhenomenologyNuclear TheoryGeneral Physics and AstronomyFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesAtlas data010306 general physicsNucleonydinfysiikkaNuclear ExperimentNuclear theoryGlauberBoson
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Asymptotic normalization of mirror states and the effect of couplings

2011

Assuming that the ratio between asymptotic normalization coefficients of mirror states is model independent, charge symmetry can be used to indirectly extract astrophysically relevant proton capture reactions on proton-rich nuclei based on information on stable isotopes. The assumption has been tested for light nuclei within the microscopic cluster model. In this work we explore the Hamiltonian independence of the ratio between asymptotic normalization coefficients of mirror states when deformation and core excitation is introduced in the system. For this purpose we consider a phenomenological rotor + N model where the valence nucleon is subject to a deformed mean field and the core is allo…

PhysicsNormalization (statistics)Nuclear and High Energy PhysicsNuclear TheoryProton010308 nuclear & particles physicsHadronFOS: Physical sciencesElementary particle01 natural sciencesNuclear Theory (nucl-th)BaryonMean field theory0103 physical sciencesAtomic physics010306 general physicsNucleonGround statePhysical Review C
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Time reversal violating Magnetic Quadrupole Moment in heavy deformed nuclei

2018

The existence of permanent electric dipole moments (EDMs) and magnetic quadrupole moments (MQMs) violate both time reversal invariance (T) and parity (P). Following the CPT theorem they also violate combined CP symmetry. Nuclear EDMs are completely screened in atoms and molecules while interaction between electrons and MQMs creates atomic and molecular EDMs which can be measured and used to test CP-violation theories. Nuclear MQMs are produced by the nucleon-nucleon T, P-odd interaction and by nucleon EDMs. In this work we study the effect of enhancement of the nuclear MQMs due to the nuclear quadrupole deformation. Using the Nilsson model we calculate the nuclear MQMs for deformed nuclei o…

PhysicsNuclear Theory010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)Atoms in moleculesHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesParity (physics)Electron01 natural sciencesDiatomic moleculePhysics - Atomic PhysicsNuclear Theory (nucl-th)DipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesQuadrupolePhysics::Atomic PhysicsAtomic physics010306 general physicsNucleonQuadrupole magnetNuclear Experiment
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Probing low-mass vector bosons with parity nonconservation and nuclear anapole moment measurements in atoms and molecules

2017

In the presence of P-violating interactions, the exchange of vector bosons between electrons and nucleons induces parity-nonconserving (PNC) effects in atoms and molecules, while the exchange of vector bosons between nucleons induces anapole moments of nuclei. We perform calculations of such vector-mediated PNC effects in Cs, Ba$^+$, Yb, Tl, Fr and Ra$^+$ using the same relativistic many-body approaches as in earlier calculations of standard-model PNC effects, but with the long-range operator of the weak interaction. We calculate nuclear anapole moments due to vector boson exchange using a simple nuclear model. From measured and predicted (within the standard model) values for the PNC ampli…

PhysicsNuclear Theory010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)Atoms in moleculesNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesParity (physics)ElectronWeak interaction01 natural sciencesVector bosonPhysics - Atomic PhysicsNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPhysics::Atomic Physics010306 general physicsNucleonNuclear ExperimentBoson
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